TW491938B - Method of designing a multichannel filtering system for measuring digital camera's spectral responsivities - Google Patents

Method of designing a multichannel filtering system for measuring digital camera's spectral responsivities Download PDF

Info

Publication number
TW491938B
TW491938B TW89125256A TW89125256A TW491938B TW 491938 B TW491938 B TW 491938B TW 89125256 A TW89125256 A TW 89125256A TW 89125256 A TW89125256 A TW 89125256A TW 491938 B TW491938 B TW 491938B
Authority
TW
Taiwan
Prior art keywords
filter
spectral
matrix
channel
filters
Prior art date
Application number
TW89125256A
Other languages
Chinese (zh)
Inventor
Gao-Wei Chang
Yung-Chang Chen
Original Assignee
Yung-Chang Chen
Gao-Wei Chang
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Yung-Chang Chen, Gao-Wei Chang filed Critical Yung-Chang Chen
Priority to TW89125256A priority Critical patent/TW491938B/en
Application granted granted Critical
Publication of TW491938B publication Critical patent/TW491938B/en

Links

Landscapes

  • Spectrometry And Color Measurement (AREA)

Abstract

For determination of camera's spectral responses, we introduce a multichannel filtering (MCF) system. The design objective of the optical system is to effectively select a limited amount of spectral (or broadband) filters to characterize the spectral features of color imaging processes, which are contaminated with noise, so that the spectral response functions can be estimated with satisfactory accuracy. In our approach, a theoretical study is first presented to pave the way for this work, and then we propose a filter selection algorithm based on the technique of orthogonal-triangular (QR) decomposition with column pivoting (QRCP), called QRCP-based method. This method involves QR computations and a column permutation process, which determines a permutation matrix to conduct the subset (or filter) selection. Experimental results reveal that the proposed technique is truly consistent with the theoretical study on filter selections. It is found that the MCF system with the filters selected from this method is much less sensitive to noise than those with other spectral filters from different selections. Thus, the spectral responsivity estimation can achieve a satisfactory accuracy.

Description

491938 五、發明說明(l) 1 · 發明背景: (一) 發明範疇: 本發明係有關於光譜響應量測系統的設計方法,特別是 針對數位取像裝置(例如,數位照相機、攝影機等裝置)之 一種光譜響應量測系統的設計方法。更特定而言,本發明 係針對量測數位取像裝置光譜響應之一種多通道濾波系統 的設計方法。 (二) 先前技術: 一般數位取像裝置的色彩訊號品質主要係由定義在可見 光範圍(4 0 0 - 7 0 0 nm )之光譜響應所決定。此光譜響應與其 光學元件、光譜濾波器(例如,紅外線截止濾波器(infrared cutoff filter)) 、 色彩濾波 器陣列 (c〇i〇r filter a r r a y )、以及影像感測器(i m a g e s e n s 〇 r )等等之光譜特性 有關。倘若已知色彩取像裝置之光譜響應,我們可以用來 4¾展β午夕重要且具經濟效益的技術與應用。例如,電腦 (機械)視覺、色彩量測與重現技術、視訊處理、樣型識 別、與彩色影像處理技術等等[丨]—[9 ]:更明確地說,我 們可以計算此裝置的色彩品質因數(c〇1〇rimetric qualify factor),此色彩品質因數係由 Neugebauer [9] 所建4的,用來表示機械視覺與人類視覺系統的光譜塑應 兩者近似的程I,即可用以決定數位相機或攝影機的:: 取像的品f,對於數位取像裝置的品質管制與分析有很大491938 V. Description of the invention (l) 1 · Background of the invention: (1) The scope of the invention: The present invention relates to the design method of a spectral response measurement system, especially for digital image pickup devices (for example, digital cameras, cameras, etc.) A method for designing a spectral response measurement system. More specifically, the present invention is a method for designing a multi-channel filtering system for measuring the spectral response of a digital imaging device. (II) Prior technology: The color signal quality of general digital image pickup devices is mainly determined by the spectral response defined in the visible light range (400-700 nm). This spectral response is related to its optical elements, spectral filters (for example, infrared cutoff filter), color filter array (color filter array), and image sensors (imager). The spectral characteristics are related. If the spectral response of the color imaging device is known, we can use it to develop important and economical technologies and applications of β Midnight. For example, computer (mechanical) vision, color measurement and reproduction technology, video processing, pattern recognition, and color image processing technology, etc. [丨] — [9]: More specifically, we can calculate the color of this device The quality factor (c0rimetric qualify factor). This color quality factor was established by Neugebauer [9] .4 It is used to represent the approximate process I of the spectral plasticity of mechanical vision and human visual system. Determining digital cameras or camcorders :: The quality f of the image to be captured is very important for the quality control and analysis of digital image capturing devices

49193.8 五、發明說明(2) 的助益。因此,量測色彩取像裝置之光譜響應是深具產業 應用價值的。 很可惜地,通常色彩取像裝置整體的光譜響應是报 難取得(即使我們可以測定影像感測元件(器)(i m a g e sensor)的光譜響應)。來自各種調查結果顯示[8],這些 視覺系統之光譜響應量測技術發展缓慢的主要原因,可歸 納如下: (1) 攝影機雜訊的存在; (2) 缺乏可製造的與價廉的色彩量度濾波器(colori 一 metric filter); (3) 光學(或色彩)濾波器在製造上的限制與困難(例如, 濾波器厚度的差異對於穿透率的影響;類似半導體製程, 此光譜響應受到色彩濾波器陣列之製程參數變動的影響很 大;因此,我們很難確定色彩通道的光譜響應是否合乎所 需的規格)。 (4 )光學組件在本質上光譜分佈的不完美(或不理想); (5)由於色彩取像多通道(muitichannel)的本性,造成光 電系統整合上的複雜度。 由於上述這些因素的存在,導致取像裝置之色彩準確度 受到相當大的限制,即使在國際間已經建立相關的色彩標 準;例如,國際照明協會(CIE)在色度學上所建議的規格 ’以及美國國家電視系統委員會(NTSC)的色彩標準[1 6 ]。49193.8 V. Benefits of Invention Description (2). Therefore, measuring the spectral response of a color imaging device is of great industrial application value. Unfortunately, usually the overall spectral response of a color imaging device is difficult to obtain (even though we can measure the spectral response of an image sensor). The results from various investigations show [8] that the main reasons for the slow development of the spectral response measurement technology of these vision systems can be summarized as follows: (1) the presence of camera noise; (2) the lack of manufacturable and inexpensive color measurements Colori-metric filter; (3) manufacturing limitations and difficulties of optical (or color) filters (for example, the effect of differences in filter thickness on transmittance; similar to semiconductor processes, this spectral response is affected by color The effect of variations in the process parameters of the filter array is significant; therefore, it is difficult to determine whether the spectral response of the color channel meets the required specifications). (4) Imperfect (or not ideal) spectral distribution of optical components in nature; (5) Due to the nature of multi-channel color imaging (muitichannel), the complexity of the integration of optoelectronic systems is caused. Due to the existence of these factors, the color accuracy of the image pickup device is quite limited, even if the relevant color standards have been established internationally; for example, the specifications recommended by the International Lighting Association (CIE) in colorimetry ' And the National Television System Committee (NTSC) color standards [16].

Abraham與Wenzel [ 3 ]在他們的美國專利中,提出一項 針對人眼色彩感知之光譜響應參數測定的技術。Takaha-Abraham and Wenzel [3] in their US patent proposed a technique for measuring the spectral response parameters of human eye color perception. Takaha-

第7頁 491938 五、發明說明(3) shi與Terashita [4]發明了一項估測傳統相機軟片光譜響 應與曝光量測定的方法。Osaki與Sugiyama [ 5 ]發表一個 色度計光譜響應的修正裝置,係根據假設的光譜響應來調 節待測色度計的輸出值,然而並未實際地量測色度計光譜 響應。此外,Zerlaut等人[6]與國際照明學會(cie)[13] 分別提出數種光輻射偵測器之光譜響應量度技術。很可惜 地,以上這些方法很難直接用來測量數位色彩取像裝置之 光譜響應。 ?〇^等人[1〇]利用干涉式濾波器(1111:61^61^1^6^1以1^ )或窄頻濾波器(narrow-band filter)來量度此一光譜變 應。這種濾波器具有分離窄波長通帶(narrow wavele^gsth band)的特性,能夠用來測量取像裝置的光譜響應。為滿 足此特性’此方法需要建構較複雜且精密的光學系統。 ^匕外,这些濾波器的價格亦遠比寬頻(或吸收式)濾波器昂Page 7 491938 V. Description of the invention (3) Shi and Terashita [4] invented a method to estimate the spectral response and exposure of traditional camera films. Osaki and Sugiyama [5] published a colorimeter spectral response correction device, which adjusts the output value of the colorimeter to be measured based on the assumed spectral response, but does not actually measure the colorimeter's spectral response. In addition, Zerlaut et al. [6] and the International Illumination Society (cie) [13] separately proposed several spectral response measurement techniques for optical radiation detectors. Unfortunately, these methods are difficult to directly measure the spectral response of digital color imaging devices. 〇 ^ et al. [1〇] used interferometric filters (1111: 61 ^ 61 ^ 1 ^ 6 ^ 1 to 1 ^) or narrow-band filters to measure this spectral change. This filter has a characteristic of separating a narrow wavelength passband (narrow wavele ^ gsth band), and can be used to measure the spectral response of an imaging device. To meet this characteristic, this method requires the construction of a more complex and sophisticated optical system. ^ In addition, these filters are also much more expensive than broadband (or absorption) filters.

旦在傳統上我們可以使用單光儀(m〇n〇chr〇mat〇r),來调 =光電巧測器(ph〇t〇-electric detect〇r}的光譜響應。 ::Ϊ緩使用’光儀或干,式濾波器 '组的實驗機構架設1 H,wyszecki [12]率先提出寬頻帶通滤波(br〇ad_ 二1k、#Λ 7Γΐη§)方法。在他的方法裏,14個光譜濾波器 見光範圍内’其穿透率分佈所形成-組線彳 二八13的條件。然而,國際照明協會(c IE ) [ 1 3 ] ·; :二St限制因素之下(例如,雜訊存在的情況),以: 濾波益組來量度感測器的光譜響應,其準確度可;Once traditionally, we can use a single light meter (m〇n〇chr〇mat〇r) to adjust the spectral response of the photoelectric sensor (ph〇t〇-electric detect〇r). The experimental mechanism of the optical instrument or dry-type filter 'set up 1 H, wyszecki [12] took the lead in proposing a wideband pass filter (br0ad_ 2 1k, # Λ 7Γΐη§) method. In his method, 14 spectra The filter sees the conditions in the range of light formed by its transmittance distribution-group line 2813. However, the International Illumination Association (c IE) [1 3] ·;: under the two St limiting factors (eg, miscellaneous Information exists), the filter response is used to measure the spectral response of the sensor, and its accuracy is acceptable;

491938 五、發明說明(4) - 會降低(因為這些濾波器在可見光範圍内的光譜穿透率彼 此相當接近地交疊著)。此外,較窄的吸收式帶通濾波已 經被窄頻帶的干涉式濾波器所取代(由於吸收式濾波器串 接組合所形成的較窄的光譜通帶會隨著整體厚度增加,而 易造成不良的穿透率)[21]。 因此,為了克服上述問題,我們建構了一套以多通道寬 頻濾波器為基礎的光譜響應量測系統[7 ],[丨4 ]。在本發 明中,我們進一步地提出一個巧妙的濾波器選擇方法,來 有效率地設計此一以濾波器為基礎的光學系統,用來降低 雜訊的效應,進而提高光譜響應量測的準確度[丨5 ]。 2. 發明概述: (一)發明目的: 本發明之目的係針對數位取像裝置提供一種光譜響應量 測系統的設計方法,來建立一套準確度高、系統結構簡 單、成本低廉的光譜響應量測系統。 〜本發明之另一目的在於設計(或選擇)一個以有限數量的# 寬頻(broadband)光譜濾波器集合為基礎之光學系統(稱為 多通道濾波(multichannel filtering (MCF))系統),用 來建立一套光譜響應量測系統,來降低此光學系統對於攝 影機雜訊的靈敏度,進而有效地估測數位取像裝置的光譜491938 V. Description of the invention (4)-will be reduced (because the spectral transmittances of these filters in the visible range overlap each other quite closely). In addition, narrower absorption band-pass filtering has been replaced by narrow-band interference filters (the narrower spectral passband formed by the series combination of absorption filters will increase with the overall thickness, which is prone to failure. Transmission rate) [21]. Therefore, in order to overcome the above problems, we constructed a set of spectral response measurement systems based on multi-channel broadband filters [7], [丨 4]. In the present invention, we further propose a clever filter selection method to efficiently design this filter-based optical system to reduce the effect of noise and thereby improve the accuracy of the spectral response measurement. [丨 5]. 2. Summary of the invention: (1) Purpose of the invention: The purpose of the present invention is to provide a method for designing a spectral response measurement system for a digital imaging device to establish a set of spectral response quantities with high accuracy, simple system structure and low cost.测 系统。 Test system. ~ Another object of the present invention is to design (or select) an optical system (called a multichannel filtering (MCF)) system based on a limited number of #broadband (broadband) spectral filter sets. Establish a spectral response measurement system to reduce the sensitivity of this optical system to camera noise, and then effectively estimate the spectrum of digital imaging devices

第9頁Page 9

49193S 五、發明說明(5) 響應。 (二)發明内容簡介: 為了達到本發明之目的,我們首先簡單地描述以一個多 通道濾波(MCF )系統,來針對數位取像裝置進行光譜響應 特徵化過程(spectral—response characterization Process)。然後引用此系統對於雜訊的靈敏度分析之結 果’來說明攝影機雜訊對於光譜響應量測準確度之影響。 此外j我們以矩陣計算理論來說明以光譜濾波器的選^來 降低系統對雜訊的靈敏度的可行性,用以進行有效率的系 統,計。由此一理論得知,在系統設計中藉由濾波器集合 的逑擇可以用來提高光譜響應估測的準確度(即降低系統 對雜訊的靈敏度)。 、 在本發明中,我們提出一個以直交三角形分解與行轉換 (orthogonal-triangular (QR) decomposition with 、 ⑶lunrn pivoting (QRCp))技術為基礎之濾波器選擇演算 =,稱為QRCP-based方法。此方法涉及一個直交三角形分 解與行排列轉換(co!umn permutati〇n)的過程,其中此 一過程決定了一個用以主導此子集合(或濾波器)^擇的 ,列矩,。貝驗的結果顯示,此一技術與所探討的濾波器 遥擇理論一致。正如我們所預期的,以此QRCP-based方法 選擇的濾波器所建構之光學系統遠比其他濾波器選擇方式 所建構的具有較佳的雜訊容忍度,使得此隱系統具有 人滿意的光譜響應估測準確度。 491938 五、發明說明(6) 3 · 技術内容: (一)詳細内容: (1)多通道濾波(MCF)系統·· 圖1顯不我們以所提出的多通道濾波(MCF)系統,來進 數位攝影機的光譜響應特徵化過程。此過程係用來產生一 、,個具有色彩白勺入射光(稱為色刺激)之集合來激勵攝影 機,使其色衫特徵能真實地從攝影機的輸出中萃取出來。 在此過程中,我們擷取色刺激在一有限區域之光輻射量空 間平均值,因此色刺激可視為波長(體“161^1^)又的函 數。此色刺激集合標記為(ς(ι),ί = 1,2,.·.,沁}用來表示其光譜功 率分佈(spectral power distribution (SPD)),單位為 W sr'1 m'2 nm4 。 來自各種實驗與調查的結果[8],[14],我們對於此系統 中待測攝影機’做了下列合理的假設: (a) 攝影機光譜響應空間分佈不均勻的程度是可以被忽略 的; (b) 沒有blooming現象發生; (c) 攝影機輸出相對於入射光信號兩者之間的關係是足夠 線性的(例如,可以將攝影機gamffla修正功能取消,即可避49193S V. Description of the invention (5) Response. (II) Brief Introduction of the Invention: In order to achieve the purpose of the present invention, we first briefly describe the use of a multi-channel filtering (MCF) system to perform a spectral-response characterization process on a digital imaging device. The results of the sensitivity analysis of this system for noise are then cited to illustrate the effect of camera noise on the accuracy of the spectral response measurement. In addition, we use matrix calculation theory to illustrate the feasibility of using a spectral filter to reduce the sensitivity of the system to noise, so as to perform an efficient system. From this theory, it is known that the selection of filter sets in system design can be used to improve the accuracy of spectral response estimation (that is, reduce the system's sensitivity to noise). In the present invention, we propose a filter selection calculus based on orthogonal-triangular (QR) decomposition with (CDlunrn pivoting (QRCp)) technology, which is called QRCP-based method. This method involves a process of orthogonal triangle decomposition and row permutation transformation (co! Umn permutation), where this process determines a column moment, which is used to dominate the selection of this subset (or filter). The results of the Bayesian test show that this technique is consistent with the filter remote selection theory discussed. As we expected, the optical system constructed by the filter selected by this QRCP-based method has far better noise tolerance than that constructed by other filter selection methods, making this hidden system have a satisfactory spectral response. Estimate accuracy. 491938 V. Description of the invention (6) 3 · Technical contents: (1) Details: (1) Multi-channel filtering (MCF) system · Figure 1 shows that we have come to the proposed multi-channel filtering (MCF) system. Characterization of the spectral response of a digital camera. This process is used to generate a collection of incident light (called color stimulus) with color to excite the camera so that its color shirt features can be truly extracted from the output of the camera. In this process, we capture the spatial average of the light radiation volume of a color stimulus in a limited area, so the color stimulus can be regarded as a function of the wavelength (body "161 ^ 1 ^). This color stimulus set is labeled ), ί = 1, 2, ..., Qin} is used to indicate its spectral power distribution (SPD), the unit is W sr'1 m'2 nm4. Results from various experiments and investigations [8 ], [14], we made the following reasonable assumptions for the camera under test in this system: (a) The degree of spatial distribution of the camera's spectral response can be ignored; (b) No blooming occurs; (c ) The relationship between the camera output and the incident light signal is sufficiently linear (for example, you can cancel the camera gamffla correction function to avoid

第11頁 491938Page 11 491938

免非線性的產生)。 此外,所有的攝影機設定或取像的參數(例如,光圈的大 小、白平衡的設定值等等)均為固定。 在此光譜響應特徵化過程中,相對於第〖個色刺激,我 們將攝衫機取像弟a個通道的輸出表示為[8 ] 心 Γς(妒 W1 +,+ 妒U: 1,2,3, 、 1 數學式(1 ) 其中’⑷是攝影機光譜響應,為暗電流所造成的偏移 量,#為攝影機雜訊[17],可見光波長範圍[λ,λ2] = [ 40 0 nm,70 0 nm],以及通道α:=ι,2,3通常表示為 RGB (red-green-blue)三個通道。在kMCF系統中,我們使 用 乂 個光譜濾波器(Spectrai f i 1 ters) (W)J = i,2,…,Nc、來 調變擴散式面光源(diffused area light source)^)所 發出的輻射光,進而產生此色刺激集合。圖2顯示此一光 源光譜功率分佈之一較佳實現例[7 ]。 考慮光源的發光面與濾波器的表面在幾何上彼此是平行 的。因此,如圖1所示,色刺激q⑷的產生可以表示成 G(又) = 5(2)/(2) ,έ=ι’2,…具。 數學式(2) 顯然地’式子(1 )能以向量(或矩陣)形式表示, ? i=\X...rNc ? i = 1,2,3, 數學式(3) 其中& =An一稱為已整修的觀察值(trimmed obser-Free from non-linearity). In addition, all camera parameters (such as aperture size, white balance setting, etc.) are fixed. In the process of characterizing the spectral response, relative to the first color stimulus, we represent the output of the camera ’s a channel as [8] heart Γς (jealous W1 +, + jealous U: 1, 2, 3, 1 Mathematical formula (1) where '⑷ is the camera's spectral response, which is the offset caused by the dark current, # is the camera noise [17], and the visible wavelength range [λ, λ2] = [40 0 nm, 70 0 nm], and channel α: = ι, 2,3 are usually expressed as three channels of RGB (red-green-blue). In the kMCF system, we use a spectral filter (Spectrai fi 1 ters) (W ) J = i, 2, ..., Nc to modulate the radiant light emitted by a diffused area light source ^) to generate this color stimulus set. Figure 2 shows a preferred implementation example of the spectral power distribution of this light source [7]. Consider that the light emitting surface of the light source and the surface of the filter are geometrically parallel to each other. Therefore, as shown in FIG. 1, the generation of the color stimulus q 可以 can be expressed as G (again) = 5 (2) / (2), έ = ι’2, ... Mathematical formula (2) Obviously 'formula (1) can be expressed in the form of a vector (or matrix),? I = \ X ... rNc? I = 1,2,3, mathematical formula (3) where & = An is called the trimmed obser-

第12頁 491938 五、發明說明(8) vation),#與A分別是表示,⑷與的~維度的列向 量,係在可見光譜範圍内以波長解析度(wavelength resolution/、作直方取樣(quadrature sampling)的樣 本數,以及上標Γ代表向量或矩陣的轉置(transp〇se)。為 了求解光譜響應向量#,~值必須為大於或等於心值, 以及考慮計算的方便,我們設定I =心。 進一步地,式子(3)可以寫成 «==(:#+/,BU3, 數學式(4) 其中向量< 佔據了色刺激矩時c 的第i列位置,即 C 2仏],以及e^xl是通道先的雜訊向量。我們很 快地觀察到代表光譜響應之向量e贫心1 ,能夠被估測出 來’如果滿足rank(C ),其中rank(_)為矩陣的秩 (matrix rank)。 (2)糸統對雜訊的靈敏度(SyStem sensitivity to η o i s e )分析 奇異值分解(singular value decomposition (SVD))在 採索矩陣結構方面,扮演一個非常重要的角色。考慮對於 矩陣』e货如存在有直交(orthogonal)矩陣// ear動與f eir-使得 數學式(5) ^TAV =diag( σι» σ2—)ePage 12 491938 V. Description of the invention (8) vation), # and A are the column vectors representing ~, and the dimensions are in the visible spectral range with wavelength resolution (quadrature) sampling), and the superscript Γ represents the transposition of the vector or matrix. In order to solve the spectral response vector #, the value of ~ must be greater than or equal to the heart value, and considering the convenience of calculation, we set I = Further, the formula (3) can be written as «== (: # + /, BU3, mathematical formula (4) where the vector < occupies the position of the i-th column of c when the color stimulation moment is occupied, that is C 2 仏] , And e ^ xl is the channel-first noise vector. We quickly observe that the vector e, which is the spectral response, is poor and can be estimated 'if rank (C) is satisfied, where rank (_) is the matrix's Matrix rank. (2) SyStem sensitivity to η oise analysis. Singular value decomposition (SVD) plays a very important role in searching the matrix structure. Consider For the matrix e Orthogonal matrix // ear movement and f eir- make mathematical formula (5) ^ TAV = diag (σι »σ2—) e

第13頁 491938 五、發明說明(9) =數,=min(w’0 ’min(·)表示取最小 值,diag(·)代表一個献《對角矩陣,與其對角線上元素 稱為奇異值。我們將矩⑽第:個大的奇異 值標記為㈣。在式子⑸中,F係由右奇異向 ht s^ngular vect0r)所形成的矩陣,我們稱之為右奇異矩 藉由奇異值分解的結果,我們介紹條件數(c〇nditi〇n number)的定義,來得到一個雜訊靈敏度的準確測度 (measure)。令方陣(stluare matrix)c ㈣是非奇異的 (n〇nsingular),mrank(c)=%,則c 的條件數,標記為 ,定義為 其中 -2(C) Μ 1^)1 = σι(〇Κ(〇 數學式(6) 數學式(7) 5(c)調2 與 %(c) =i/||(c)l 以及丨卜«2表示矩陣(或向量)的模方值(2_n〇rm) [18]。如果 以c) a 1是相對地小,通稱為well—c〇nditi〇ned。Page 13 491938 V. Explanation of the invention (9) = number, = min (w'0 'min (·) means taking the minimum value, diag (·) represents a diagonal matrix, and the elements on its diagonal are called singular Value. We label the moment ⑽: the large singular value as ㈣. In the expression ⑸, F is a matrix formed by the right singularity ht s ^ ^ ular vect0r), we call it the right singular moment by singularity As a result of the value decomposition, we introduce the definition of the condition number to obtain an accurate measure of noise sensitivity. Let the square matrix (clu) be non-singular, and mrank (c) =%, then the condition number of c is marked as, where -2 (C) M 1 ^) 1 = σι (〇 Κ (〇 Mathematical formula (6) Mathematical formula (7) 5 (c) Tune 2 and% (c) = i / || (c) l and 丨 2 «2 represents the modulus value of the matrix (or vector) (2_n 〇rm) [18]. If c) a 1 is relatively small, it is commonly known as well-contained.

在此MCF系統中,為了減少雜訊的效應,我們似乎可以 重複地觀察攝影機的輪出,來取得較多的訊息,然後藉由 一般數位估測,術來計算光譜響應函數(或向量)。然而, 此一作法是不實際的,因為較多的觀察會造成光譜響應特 徵化更加地耗費時間。在從式子(4)得知,藉由矩陣計算In this MCF system, in order to reduce the effect of noise, it seems that we can repeatedly observe the rotation of the camera to obtain more information, and then use ordinary digital estimation to calculate the spectral response function (or vector). However, this approach is impractical because more observations can cause the characterization of the spectral response to be more time consuming. It is known from equation (4) that by matrix calculation

第14頁 五、發明說明(10) 理論我們可以證明如果矩陣C的條件數h(c)是足夠的小, 則光譜響應向量的估測能具有相當令人滿意的準確度,此 一結果係由於此系統儘可能對於雜訊不靈敏的緣故[i 5 ], [18,疋理2·7·2 與引理(Lemma)2.7 1]。 從式子(2)與(4),我們發現在—已知的光源之下,對應 於色刺激的光譜濾波器決定了此Mcf系統的結構以及系統 對雜訊的靈敏度。明確地說,適當地選擇濾波器能夠使得 矩陣C最小的特徵值%(C)變得足夠地大,以及根據此一 結果MO = a1(C)AMC)會變得儘可能地小,其 中 =||C||2 係與色刺激集合的總功率有關,由於色刺激的寬頻性質, 此巧⑺值是侷限於某一相對地有限的範圍内(即bounded) 。因此’濾波器的選擇對於光譜響應估測的準確度以及系 統對雜訊的靈敏度是非常重要的。 (3)有效率的MCF系統設計 (a)光譜濾波器選擇的理論探討 由上述可知’寬頻的色刺激信號能藉由直方取樣以波 長解析度~ =心為維度的向量來表示。一般而言,一個巨 大的色刺激集合能夠以一個具有行分割(c〇lumn partitioning) 的矩陣j € sr" 來表示 ,其中„ a 乂為 這些色 刺激的 數量,以及波長解析度。很清楚地,矩呻 的每一個行向量(column vector)代表個別的色刺激。 1Page 14 V. Description of the invention (10) Theory We can prove that if the condition number h (c) of the matrix C is sufficiently small, the estimation of the spectral response vector can have quite satisfactory accuracy. This result is Because this system is as insensitive to noise as possible [i 5], [18, theorem 2 · 7 · 2 and Lemma 2.7 1]. From equations (2) and (4), we find that under the known light source, the spectral filter corresponding to the color stimulus determines the structure of this Mcf system and the sensitivity of the system to noise. Specifically, proper selection of the filter can make the minimum eigenvalue% (C) of the matrix C sufficiently large, and according to this result MO = a1 (C) AMC) will become as small as possible, where = || C || 2 is related to the total power of the color stimulus set. Due to the broadband nature of the color stimulus, this value is limited to a relatively limited range (ie bounded). Therefore, the choice of the 'filter is very important for the accuracy of the spectral response estimation and the sensitivity of the system to noise. (3) Design of efficient MCF system (a) Theoretical discussion of spectral filter selection From the above, it can be known that the 'wide-band color stimulus signal' can be represented by a histogram of a vector with a wavelength resolution of ~ = heart. In general, a huge set of color stimuli can be represented by a matrix j € sr " with row partitioning, where a a 乂 is the number of these color stimuli and the wavelength resolution. It is clear , Each column vector of the moment 代表 represents an individual color stimulus. 1

第15頁 49193.8 五、發明說明(11) 在此矩陣2中任意挑選乂個行向量所形成的子矩陣 (submatrix)可視為一個色刺激子集合的實現或者視為對 應於色刺激的一種光譜濾波器選擇結果之實現。對於子集 合選擇(subset selection),我們以下簡述一項在矩陣計 算理論中涉及排列矩陣(permutati〇n matrix)的重要結果 [18]。考慮式子(5)得到的j e 的奇異值分解(SVD), 們有j之右奇異矩陣 F: ^-Nc 其中rankU )乏\ 。定義乓,藉由 數學式(8 ) ι-ΝζPage 15 49193.8 V. Description of the invention (11) In this matrix 2, a submatrix formed by arbitrarily selecting a row vector can be regarded as the realization of a set of color stimuli or regarded as a kind of spectral filtering corresponding to color stimuli Implementation of the device selection result. For subset selection, we briefly describe an important result involving permutation matrix in matrix calculation theory [18]. Considering the singular value decomposition (SVD) of j e obtained by equation (5), we have the right singular matrix F of j: ^ -Nc where rankU) is lacking. Define ping pong, with the formula (8) ι-Νζ

其中/> 是 FVWhere / > is FV

Vn VnΛ 4 Nc n^Nc 數學式(9) 個排列矩陣(permutati〇n matrix)。令 η-Μ 〃 數學式(1 〇 ) 以及如果Κ是非奇異的(n〇nsingular),則我們有 σ^(Α)/ψ\\ I < ^ σ^(,ίΐ)。 數與、 從式子(8)至(li)可知,排列矩陣ρ在子集合 器)選擇上扮演—個非常重要的角色。此矩陣記(錄‘慮二皮 串的行互換(column interchange)的動作。例如,連目 要互換矩陣的第2行與第3行。我 來Μ以。,與4這兩行互換所形成的矩 $王 卞”"』可以表Vn VnΛ 4 Nc n ^ Nc Mathematical formula (9) Permutation matrix. Let η-Μ 〃 mathematical formula (10) and if κ is nonsingular, we have σ ^ (Α) / ψ \\ I < ^ σ ^ (, ίΐ). From the equations (8) to (li), we know that the permutation matrix ρ plays a very important role in the selection of the subcollector. This matrix records the action of column interchange of the second string. For example, the second row and the third row of the matrix are to be interchanged at the same time. I come to M, and it is formed by the two rows interchanged with 4. Moment $ 王 卞 "can be expressed

五、發明說明(12) 示成叫,即為一個矩❼的行轉換表示式 互換能夠以一個排列矩陣C ^ π" ,、中垃個仃 純地將單位矩陣(identi •勺運斤來表示。藉由單 [拖曲枘叮 Υ matrix)’e #"的第2行盥第3行V. Description of the invention (12) Shown as a name, that is, a row transformation expression of a moment ❼ can be expressed as a permutation matrix C ^ π " 。By single [Tow song 枘 ΥΥ matrix) 'e # " line 2 and line 3

互換,我們可以得到這個矩陣^内容。、—VI 於一連串的排列矩陣P| p v也,對應 能夠以-個排列矩陣 1气…叫來表示。 在式子(9 )中,矩陣/>番報 戈庠# ^ ^ , ’排了矩陣4之行(column)的 個r / Ί中1們4求的子矩陣€心出現在#的前面乂 個仃(column),以及剩餘6W r ® ”勺仃(column)所形成的區塊標記 為A 。針對式子(4 ),游Μ AW __ b· 對地大的值。 我^c =年,以及假設π)具有相 從式子⑹、(10)、與⑴),貞們了解到決定排列矩陣 二能夠使得IMU冰)儘可能地小,亦即使得⑽)足夠地 趣近㈣。此-結果藉由奇異值分解(svd)的運算,我們 可知 =、(〇=训會變得足夠大,亦即⑽會變得足 夠小。因此,決定矩陣*是遽波器(或子集合)選擇的關 (b)濾波器選擇的演算法設計 在矩陣計算理論中[1 8 ],我們發現qRCP方法是一個有效 決定矩陣P的方法,使得或式子(11)中的阼I變得足 夠小。然後基於此方法,我們發展出QRCp_based方法來選 491938 五、發明說明(13) 擇所欲得到的有限數量的光譜濾波器集合,用以建構此 MCF系統’來降低系統對雜訊的靈敏度,進而提高光譜響 應量測的準確度。 (i) QRCP 方法: 考慮一個矩陣的直交三角形(QR)分解為 ^ G =职 or QrG 數學式(12) 使得矩陣0€旷是直交的㈠“匕叫⑽以)以及矩陣“矿η是 上二角形的(upper-triangular),其中”與《均為整數。 此⑽“方法包含了QR分解與行排列轉換(c〇lumn pivoting or column permutati〇n)。對於行轉換而言,一連串的行 互換動作會使得具有較小模方值(2-nonn)的行(column)向 此矩陣右邊的角落移動。此外,對於QR分解而古,一連串 的行排列轉換的步驟與反射運算子(ref lect〇r)(即 轉換(transfc)rmatic)n))相結合。關於QRCP 運 开的砰細描述,請參閱參考文獻[丨8 ] 〇 來自式子(8),我們令Reciprocally, we can get the contents of this matrix ^. , —VI also corresponds to a series of permutation matrices P | p v, which can be represented by a permutation matrix 1 Qi ... In the expression (9), the matrix / > 番 报 戈 庠 # ^ ^, 'the submatrix of 1 and 4 in the rows r / 排 of the matrix 4 (column) appears in front of # A block formed by a single column and the remaining 6W r ® "column" is marked as A. For formula (4), you can move AW __ b · a large value to the ground. I ^ c = Years, and assuming that π) has coherent expressions ⑹, (10), and ⑴), the zhen learned that the decision to arrange matrix two can make IMU ice) as small as possible, that is, ⑽) is sufficiently interesting. This-result through the operation of singular value decomposition (svd), we can know that =, (〇 = training will become large enough, that is, ⑽ will become small enough. Therefore, the decision matrix * is a wavelet (or a subset) (B) The algorithm of filter selection is designed in the matrix calculation theory [1 8]. We found that the qRCP method is an effective method to determine the matrix P, so that 阼 I in OR (11) becomes Small enough. Then based on this method, we developed the QRCp_based method to select 491938. V. Description of the invention (13) Choose the finite number of spectral filters you want It is used to construct this MCF system to reduce the system's sensitivity to noise and improve the accuracy of spectral response measurement. (I) QRCP method: Consider the orthogonal triangle (QR) of a matrix decomposed into ^ G = duty or QrG Mathematical formula (12) makes the matrix 0 旷 is orthogonal ㈠ "dagger ⑽" and the matrix "mine η is upper-triangular, where" and "are integers. This "method" includes QR decomposition and row permutation (column pivoting or column permutati). For row conversion, a series of row swapping actions will result in rows with smaller non-square values (2-nonn). (Column) moves to the right corner of this matrix. In addition, for QR decomposition and ancient times, a series of steps of row permutation conversion are combined with reflection operator (transfc) rmatic n)). For a detailed description of the operation of QRCP, please refer to the reference [丨 8] 〇From formula (8), let us

Vr- 數學式(13) 數學式(14) 、上三角矩 將QRCP方法運作在γ上,得到 er [K ]P =Vr- Mathematical formula (13) Mathematical formula (14), upper triangle moment Operate QRCP method on γ, get er [K] P =

Nz n, /、中直父二角形矩陣ρ 、排列矩陣^ 491938 五、發明說明(14) 陣A ㈣、以及义是一個义X卜W矩陣。對於子集合(或 濾波器)選擇而言,矩陣心扮演一個很重要的角色。 一 我們將主對角線上的元素標記為片,hi,2,,% ,其中 凡〇因為二角形矩陣!?!,是非奇異的(n〇nsingular)。由於 來自矩陣/^所造成的行互換(column interchange)的效 應,片的絕對值,即kl,hU,.·.,乂,會變得相對的大,此 一結果導致的行向量(c〇lumn vector)是很明顯地相互 獨立。藉由SVD運算發現^&)對〇·,#,)的比值,即&况), 是足夠小的。因此,此行排列轉換的過程會使得义為儘可 能地 well- conditioned 〇 來自式子(10)與(14),針對矻我們有 ίκ,Ί =ρτ X" k.' L從 0 數學式(1 5 ) 由於直父(〇 r t h 〇 g ο n a 1 )性質6r0 ,我們可以證明 數學式(16) [18,ρ· 574]。由式子(6)、(7)、與(16)可得 輕‘L 取_1 .數學式(i 7) 因為^是儘可能地^^11-〇011(^1^0116(1,以及#〇對<^1|) 的比值是有界的(b 〇 u n d e d ),所以會變得相當地 we 11-conditioned;即6欠,)或,IL是足夠小的。因此,此Nz n, /, middle-right parent diagonal matrix ρ, permutation matrix ^ 491938 V. Description of the invention (14) Matrix A ㈣, and meaning is a meaning X and W matrix. For sub-set (or filter) selection, the matrix heart plays an important role. 1. We label the elements on the main diagonal as slices, hi, 2 ,,%, where Fan 0 is non-singular because of the two-sided matrix!?!. Due to the column interchange effect caused by the matrix / ^, the absolute value of the slice, that is, kl, hU, .., 乂, will become relatively large. The row vector (c lumn vector) is obviously independent of each other. Through SVD calculation, it is found that the ratio of ^ &) to 〇, #,), that is, & condition), is sufficiently small. Therefore, the process of permutation and transformation of this line will make the meaning as well-conditioned as possible. From the formulas (10) and (14), for 矻 we have ίκ, Ί = ρτ X " k. 'L from 0 mathematical formula ( 1 5) Due to the nature of the direct parent (〇rth 〇g ο na 1) 6r0, we can prove the mathematical formula (16) [18, ρ · 574]. From formulas (6), (7), and (16), we can get the light 'L to take _1. Mathematical formula (i 7) because ^ is as much as possible ^^ 11-〇011 (^ 1 ^ 0116 (1, And the ratio of # 〇 to < ^ 1 |) is bounded (b 0unded), so it will become quite 11-conditioned; that is, 6 under, or IL is small enough. So this

第19頁 491938 五、發明說明(15) -- QRCP方法是—個有效的子集合(或濾波器)選擇方法。 (i i) QRCP-based 方法: 我們將上述QRCp方法在子集合(或濾波器)選擇上的效 應’總結為5項歸納點(inducti〇n),如圖3所示。依據因 果關係,這些歸納點可以整理如下·· 歸納1 :取不之QRCP運算; 歸納2 ·使得%洱,)變得足夠地小,其中A為上三角矩陣; 歸納3 :導致5%)與IPl充分地減少(由式子(丨7)得知); 歸納4 :使得值變得足夠地大; 歸納5 ·由式子(11)可知,〜(成)會接近〇〜(』)。 如果%⑼是足夠大的,則= 能夠充分地被增 大。因此,如式子(4)所示,以此方法所選擇的光譜濾波 為iMCF糸統會對於雜訊儘可能地不靈敏。本發明中,我 們提出一以QRCP為基礎的濾波器選擇演算法,稱為 QRCP-based方法。 如前面所述,矩陣J € 係由具有波長解析度^的” 個色刺激之光譜功率分佈(SPD)所形成,其中H = #。 了識別此#個待選的濾波器,我們將它們分別標上渡波器 索引編號(filter index number) 1,2, ···,#,並且令 遽波為、索弓丨向里(filter index vector) =[12 € s^h| 代表這些濾波器依數值次序的集合。我們所提的Page 19 491938 V. Description of the invention (15)-The QRCP method is an effective method for selecting a subset (or filter). (i i) QRCP-based method: We summarize the effect of the above QRCp method on the selection of subsets (or filters) as five inductive points, as shown in Figure 3. According to the causal relationship, these induction points can be arranged as follows: • Induction 1: QRCP operation that cannot be taken; Induction 2 • makes% 洱,) sufficiently small, where A is the upper triangular matrix; induction 3: leads to 5%) and IPl is sufficiently reduced (as known from Equation (7)); Induction 4: makes the value sufficiently large; Induction 5 • As can be seen from Equation (11), ~ (成) will be close to 0 ~ (『). If% ⑼ is large enough, = can be sufficiently increased. Therefore, as shown in equation (4), the spectral filtering selected by this method as the iMCF system will be as insensitive to noise as possible. In the present invention, we propose a QRCP-based filter selection algorithm, called the QRCP-based method. As mentioned earlier, the matrix J € is formed by the spectral power distribution (SPD) of "color" stimuli with wavelength resolution ^, where H = #. To identify these # candidate filters, we will separate them Mark the filter index number (filter index number) 1,2, ···, #, and let the wave wave be, and the cable bow 丨 inward (filter index vector) = [12 € s ^ h | A collection of numerical order. What we mentioned

491938 五、發明說明(16) QRCP-based濾波器選擇演算法如圖4所示, 濾波器選擇演算法: 餘欽速如下· 步驟1 :陣4的SVD運算,並儲存矩陣p,如式子(5) 步驟2:檢驗是否滿足rank(jlw ?若為是(Yes), 行下一步驟。若為非(N〇),則結束工作。、 步驟3:取K矩陣内义個行(c〇lumn),來建構子矩鲈, 此K稱之為右奇異子矩陣。 步驟4:取C之QRCP運算,並儲存排列矩呻p。 步驟L令<々,其中<esr是一個轉置的(trans一 posed)濾波器索引向量作行排列轉 )所形成的向量’以及。指定向量d,前面乂個 $:來形成向量f,這些义個元素即為所選擇的濾 波态索引編號(selected filter index number)。因此。, <被稱為所選擇的濾波器索引向量(selected index vector) 。 Γ 隶後’結束工作(e n d)。491938 V. Description of the invention (16) The QRCP-based filter selection algorithm is shown in Figure 4. The filter selection algorithm: Yu Qinsu is as follows. Step 1: The SVD operation of matrix 4 and stores the matrix p, as in the formula (5) Step 2: Check whether rank (jlw is satisfied. If yes, go to the next step. If it is not (N0), end the work. Step 3: Take the rows in the K matrix (c 〇lumn), to construct the sub-moment bass, this K is called the right singular sub-matrix. Step 4: Take the QRCP operation of C, and store the permutation moment 呻 p. Step L Lets < The vector formed by the trans-posed filter index vector is arranged in rows. Specify the vector d, followed by a $: to form the vector f. These elements are the selected filter index number. therefore. , ≪ is called the selected filter index vector (selected index vector). Γ followed by the work (e n d).

(二)較佳實現例: 我們採用# =135個Roscolux光譜濾波器來建構此巨大的 色刺激矩陣2 。使用此QRCP-based演算法,我們得到(B) Preferred implementation example: We use # = 135 Roscolux spectral filters to construct this huge color stimulation matrix 2. Using this QRCP-based algorithm, we get

第21頁 491938Page 21 491938

H4個選擇的渡波器[15],其光譜穿透率分佈如圖 示。這些所選擇的渡波器之索引編號以粗 的第2行。 4 衣丄 (1)光譜響應函數(或向量)的估測 光譜響應向量妒蚌U3)的元素值在實際上均為非負數 (nonnegative),即此限制可表示為 、 ^ ^>0 A:=l,2,3 〇 、 ’ 數學式(18) 來自式子(4 ),為了得到在最小平方誤差觀點下之光譜響 應向量估測的最佳解,標記為{i(*U = U3},我們採用 Lawson and Hanson [19]所提的NNLS (n〇nnegative least squares)演算法,解下列的NNLS問題: 最小化(m i n i m i z e ) lCsiA) , 數學式(19) 滿足夕)20, 其中光譜響應估測向量⑼U = US}為乂 xi的向量。H4 selected wavelet [15], its spectral transmittance distribution is shown in the figure. The index numbers of these selected ferrules are shown in bold line 2. 4 Yi (1) The estimated spectral response function (or vector) of the spectral response vector (element U3) is actually nonnegative, that is, this limit can be expressed as, ^ ^ > 0 A : = L, 2,3 〇, 'Mathematical formula (18) is derived from formula (4), in order to obtain the best solution of the spectral response vector estimation from the viewpoint of the least square error, mark {i (* U = U3 }, We use the NNLS (n0nnegative least squares) algorithm proposed by Lawson and Hanson [19] to solve the following NNLS problem: minimize (lCsiA), mathematical formula (19) satisfies evening) 20, where the spectrum The response estimation vector ⑼U = US} is a vector of 乂 xi.

根據估測所得的光譜響應向量w ,我們可以在適當的 假汉之下使用元美重建(perfect reconstruction)或向上 取樣(upsampling)技術[7],[20],即低通濾波(i〇w〜 pass filtering)技術,來得到具有我們所欲的波長解析 度之光譜響應。圖6顯示估測的Sony XC711攝影機光 譜響應(波長解析度為5 n m )。Based on the estimated spectral response vector w, we can use perfect reconstruction or upsampling techniques [7], [20], ie, low-pass filtering (i0w) ~ Pass filtering) technology to get a spectral response with the desired wavelength resolution. Figure 6 shows the estimated spectral response of the Sony XC711 camera (wavelength resolution of 5 nm).

第22頁 491938 五、發明說明(18) (2 ) 雜訊效應的檢驗:以不同的濾波器選擇法之估測、结 果為例Page 22 491938 V. Description of the invention (18) (2) Examination of noise effect: Taking the estimation and results of different filter selection methods as examples

為了驗證此QRCP-based方法優於其他的選擇方法,我們 考慮其他三種不同的濾波器組選擇結果,分別標記為選_ 法 1 (selection 1)、選擇法2 (selection 2)、與選擇法 3 ( se 1 ec t i on 3 )。它們的濾波器索引編號分別如表1的第 3、4、5行所示。在此表中,由QRCP-based方法所選出的 濾波器,其索引編號均以粗黑體表示。選擇法1係以—個 相異的濾波器(例如索引編號15),來取代由QRCP-based方 法所選出的濾波器集合中的一個。此相異的濾波器之索^丨 編號我們劃上底線用來表示此濾波器與QRCP — based方法所 選出的不同。同理,選擇法2所選出的濾波器與此方法所 選出的有半數不同,以及選擇法3與此方法所選出的完全 不同。 表2顯示我們的實驗結果與上述的濾波器選擇理論一 致,即滿足式子(11) s £、⑼的關係。表3 比較來自不同濾波器選擇所得的條件數(condition " numbers)。顯然地,QRCP — based方法所得的條件數最小, ,示以此方法選擇的濾波器集合所建構的KF系統,其光 譜響應估測之結果最不受雜訊的影響。 為了檢驗在不同訊號雜訊比(signal_t〇_n〇ise rati〇 (SNR))之下雜訊的效應,我們以圖6所估測的光譜響應來 模擬攝影機的光譜響應(simuUted spectraiIn order to verify that this QRCP-based method is superior to other selection methods, we consider three other different filter bank selection results, which are labeled as selection_1, selection2, and selection3. (se 1 ec ti on 3). Their filter index numbers are shown in lines 3, 4, and 5 of Table 1, respectively. In this table, the index numbers of the filters selected by the QRCP-based method are shown in bold bold. Selection method 1 replaces one of the filter sets selected by the QRCP-based method with a different filter (for example, index number 15). The number of this different filter ^ 丨 We underline the number to indicate that this filter is different from the one selected by the QRCP — based method. In the same way, the filter selected by selection method 2 is half different from the one selected by this method, and the selection method 3 is completely different from this method. Table 2 shows that our experimental results are consistent with the above-mentioned filter selection theory, that is, satisfying the relationship of equations (11) s £ and ⑼. Table 3 compares condition " numbers from different filter selections. Obviously, the condition number obtained by QRCP-based method is the smallest, which shows that the KF system constructed by the filter set selected by this method has the least spectral noise estimation result. In order to test the effect of noise under different signal-to-noise ratios (signal_t〇_n〇ise rati〇 (SNR)), we use the spectral response estimated in Figure 6 to simulate the camera's spectral response (simuUted spectrai

491938491938

responsivi ties),並考慮在使用大約8位元的影像擷取系 統之下’系統所可能具有的信號雜訊比分別為3 〇、3 5、 40、與4 5 dB [22]。表4顯示以QRCP-based方法選出的滤 波器集合所建構的MCF系統,在各個不同的SNR比值之下其 正體的規一化均方根誤差(〇veraH n〇rmaiized root-mean-square error (NRMSE))均小於其他渡波器選 擇的結果。以SNR 35 dB為例,如圖8(d)與8(a)、8(b)、 8(c)相比較,qrcp —based方法所得到估測的(estimated) 與模擬的(simulated)光譜響應兩者誤差最小(相較於其他 選擇法1、2、與3所建構之MCF系統做光譜響應估測之結 果)。因此’我們可以看到此方法在理論、模擬、與實驗 上所得的結果均優於其他的濾波器選擇法。responsivi ties), and considering the use of approximately 8-bit image capture systems, the signal-to-noise ratios that the system may have are 30, 35, 40, and 4 5 dB [22]. Table 4 shows the normalized root-mean-square error (〇veraH n〇rmaiized root-mean-square error) of the MCF system constructed by the filter set selected by the QRCP-based method under different SNR ratios. NRMSE)) are all smaller than the results of other wave filter choices. Taking SNR 35 dB as an example, as shown in Fig. 8 (d) and 8 (a), 8 (b), 8 (c), the estimated and simulated spectra obtained by the qrcp-based method are compared. The response has the smallest error (compared to the results of spectral response estimation of MCF systems constructed by other selection methods 1, 2, and 3). Therefore, we can see that the theoretical, simulation, and experimental results of this method are better than other filter selection methods.

(3 )光譜響應估測性能(或誤差)驗證 為了計算光譜響應估測誤差,我們以國際照明協會 (CIE)所建議的〇/45色彩量測架構[21 ]為基礎,提出一個 色彩測減與 1度(〇:〇1〇]: testing and measurement (C Τ Μ ))組悲’來產生7 2種不同的測試色光(七e s七i n g colored 1 ight (TCL))。此測試色光的集合係由3種不同 的光源(分別為 i 素燈(tungsten halogen lamp (THL))色 溫3 200 K、日光型照明體D55、與D65),來配合Macbeth Color Checker (MCC)包含的24個標準色片所產生的。 圖7顯示相對於測試色光(TCL )編號1至72的規一化均方 根誤差(NRMSE)分佈。表5列出在此CTM組態之下,來自不(3) Verification of spectral response estimation performance (or error) In order to calculate the spectral response estimation error, we propose a color measurement subtraction based on the 0/45 color measurement architecture [21] proposed by the International Lighting Association (CIE). With 1 degree (〇: 〇〇〇): testing and measurement (C T M)) group to generate 7 2 different test color light (seven es seven ing colored 1 ight (TCL)). This test color light collection consists of 3 different light sources (tungsten halogen lamp (THL)) with a color temperature of 3 200 K, daylight-type illuminators D55, and D65, to complement the Macbeth Color Checker (MCC). Of 24 standard color films. Figure 7 shows the normalized root mean square error (NRMSE) distribution with respect to test color light (TCL) numbers 1 to 72. Table 5 lists under this CTM configuration.

=波器選擇所得的光譜響應估測誤差 的規-化均方根誤差(Qverall NRMSE)的定義b為表中’正體 |ςΣ 2 (Ww γ / W3=l . 其中 是估測的攝影機輸出值帛欠于式(2〇) 光的光譜功率分佑以月已知的釦個測試色 力羊刀:以及估測所得的光譜響應,配合式子 。在表V:到)/」為實際的攝影機輸出值,以及〜=72 隼人^建構看到了以帆卜以㈣方法選擇的滤波器 二匕均方I 】 得到的所有色彩通道之光譜響應規 中最大相 值MSE)都小於〇.022,以及在這些通道 中取大規一化估測誤差值(maximum normalized estimation err〇r)為〇〇4〇25 。 4 ·功效與特點: 本發明與先前技術之比較如下:= The definition of the normalized root-mean-square error (Qverall NRMSE) of the spectral response estimation error obtained by the wave filter selection is b 'in the table,' orth | | Σ 2 (Ww γ / W3 = l. Where is the estimated camera output value帛 Under the formula (20), the spectral power of the light is measured by a known color power sheep knife: and the estimated spectral response is matched with the formula. In Table V: to) / "is the actual The camera output value and ~ = 72 = person ^ construction saw that the filter selected by the fan method ㈣ 均 mean square I】 obtained by the maximum phase value of all color channels in the spectral response gauge (MSE) are less than 0.022, And in these channels, the normalized estimation error (maximum normalized estimation err) is taken to be 0.000425. 4 · Efficacy and Features: The comparison between the present invention and the prior art is as follows:

(、>一)我們提出一套以多通道(寬頻)濾波器集合為基礎的 光譜響應量測系統(即MCF系統),此系統遠比具有窄頻干 /步式濾、波為或單頻光譜儀(111〇11〇^]:〇111^〇1^)的系統便宜許 多’以及我們的方法大幅地簡化傳統光譜響應量測系統的 硬體複雜度。 (二)我們發展出一個以直交三角形分解與行轉換(QRCP)(, ≫ a) We propose a set of spectral response measurement system (ie MCF system) based on a multi-channel (wideband) filter set. This system is much better than a narrow-band dry / step filter, wave filter or single filter. Frequency spectrometer (111〇11〇 ^]: 〇111 ^ 〇1 ^) system is much cheaper 'and our method greatly simplifies the hardware complexity of traditional spectral response measurement systems. (B) We have developed a QRCP

第25頁Page 25

=法為基礎的濾波選擇演算法,即QRCp — based方法, 有效率地設計此一MCF系統。 木 -在本發明中,以QRCP-based方法選擇的濾波器集人 建構之MCF系統會比其他方法所建構之MCF系統,具有 的雜訊靈敏度,即對於光譜響應量測具有較高的準乂 四 在本舍明之貫施例中,以QRCP-based方法選擇的濾 波器集合所建構的MCF系統得到的所有色彩通道之光譜塑 應規一化均方根誤差值(NRMSE)都小於〇 〇22,以及在這曰些 通道中最大規一化估測誤差值為〇. 〇 4 〇 2 5。 本發明之附圖及說明文字之中已揭示了本發明的較佳實施 例’雖然其中應用了特定條件,但只用來廣泛地說明本發 明’並非用來限制本發明。本發明的範圍係界定於後述的 申請專利範圍乙節之内。 5 ·參考文獻: (專利文獻) [1] Y. Okui, s. Ito, and M. Sugiyama,= Method-based filtering selection algorithm, QRCp — based method, to efficiently design this MCF system. -In the present invention, the filter set selected by the QRCP-based method is more noise-sensitive than the MCF system constructed by other methods, that is, it has a higher accuracy for spectral response measurement. Fourth, in this embodiment of Ben Sheming, the spectral plasticization normalized root mean square error value (NRMSE) of all color channels obtained by the MCF system constructed by the filter set selected by the QRCP-based method is less than 〇22 , And the maximum normalized estimation error value in these channels is 0.004 〇 2 5. The drawings and the description of the present invention have disclosed a preferred embodiment of the present invention ', although specific conditions are applied therein, but are only used to broadly explain the present invention' and are not intended to limit the present invention. The scope of the present invention is defined in section B of the patent application scope described later. 5 · References: (Patent Literature) [1] Y. Okui, s. Ito, and M. Sugiyama,

Multi-channel spectral light measuring device, US Patent No.; 4909633, issued date: March 20, 1 99 0.Multi-channel spectral light measuring device, US Patent No .; 4909633, issued date: March 20, 1 99 0.

第26頁 491938 五、發明說明(22) [2] B. Larsen, "Color camera system having complete spectral characteristics,丨’ US Patent No. 3789132, issued date: Jan· 29, 1974.Page 26 491938 V. Description of the invention (22) [2] B. Larsen, " Color camera system having complete spectral characteristics, ' US Patent No. 3789132, issued date: Jan 29, 1974.

[3] G. Abraham and G. Wenzel, "Method and apparatus for determining spectral sensitivity parameters of color-sensitive receptors in the eye," US Patent No.: 5801808, issued date: Sept. 1, 1998.[3] G. Abraham and G. Wenzel, " Method and apparatus for determining spectral sensitivity parameters of color-sensitive receptors in the eye, " US Patent No .: 5801808, issued date: Sept. 1, 1998.

[4] K. Takahashi and T. Terash i ta, ”Method of estimating spectral distribution of film and method of determining exposure amount,M US Patent No.: 5671060, issued date: Sept. 23, 1997.[4] K. Takahashi and T. Terashita, ”Method of estimating spectral distribution of film and method of determining exposure amount, M US Patent No .: 5671060, issued date: Sept. 23, 1997.

[5] S. Osaki and M. Sugiyama, ’丨 Spectral sensitivity correcting device in a photoelectric tristimulus colorimeter," US Patent No.: 4989982, issued date: Feb. 5, 1991.[5] S. Osaki and M. Sugiyama, ’丨 Spectral sensitivity correcting device in a photoelectric tristimulus colorimeter, " US Patent No .: 4989982, issued date: Feb. 5, 1991.

[6] G. A. Zerlaut, R. D. Whitaker, and A. W.[6] G. A. Zerlaut, R. D. Whitaker, and A. W.

Purnell, " Method and apparatus for determining spectral response and spectral response mismatch between photovoltaic devices,丨’ US Patent No.: 4467438, issued date: Aug· 21, 1984· [7] G. W. Chang and Y. C. Chen, "Automatic Spectral Respons i v i ty Measurement System for Color Video Cameras, n (數位色彩取像裝置之自動化光譜響應Purnell, " Method and apparatus for determining spectral response and spectral response mismatch between photovoltaic devices, 丨 'US Patent No .: 4467438, issued date: Aug · 21, 1984 · [7] GW Chang and YC Chen, " Automatic Spectral Respons ivi ty Measurement System for Color Video Cameras, n (Automated Spectral Response of Digital Color Imaging Device

第27頁 491938 五、發明說明(23) 量測方法與系統),F i 1 e d t 〇 R 0 C P a t e n t (N 〇. 88109743, June 10, 1999)· (技術資料與論文) [8] G. Sharma,Η· J· Trussell,’’Digital color imaging,丨丨 IEEE Trans. Image Processing, vo 1. 6, no. 7,pp. 90 1 - 932,1 997.Page 27, 491938 V. Description of the invention (23) Measurement method and system), F i 1 edt 〇R 0 CP atent (N 〇 88109743, June 10, 1999) · (Technical data and papers) [8] G. Sharma, J. Trussell, `` Digital color imaging, IEEE Trans. Image Processing, vo 1. 6, no. 7, pp. 90 1-932, 1 997.

[9] J. A. C. Yule, Principles of Co lor Reproduction, NY: John Wiley and Sons, 1967. (reprinted in 1989) [10] S. 0. Park et a 1. , "Development of spectral sensitivity measurement system of image sensor devices," Proc. of IS&T/SID 1995 Color Imaging C ο n f. : Col or Science,System and Appls·, pp· 115-118, 1995.[9] JAC Yule, Principles of Co lor Reproduction, NY: John Wiley and Sons, 1967. (reprinted in 1989) [10] S. 0. Park et a 1., " Development of spectral sensitivity measurement system of image sensor devices, " Proc. of IS & T / SID 1995 Color Imaging C ο n f.: Col or Science, System and Appls ·, pp · 115-118, 1995.

[11] P. M. Hubei et a 1., "A comparison of methods of sensor spectral sensitivity estimation,M Proc. of IS&T/SID 1994 Color Imaging Conf.: Color Science, System and Appls, pp. 45-48, 1994.[11] PM Hubei et a 1., " A comparison of methods of sensor spectral sensitivity estimation, M Proc. Of IS & T / SID 1994 Color Imaging Conf .: Color Science, System and Appls, pp. 45-48, 1994.

[12] G· Wyszecki,'丨 Multifilter method for determining relative spectral sensitivity functions of photoelectric detectors,M J. Opt.[12] G. Wyszecki, '丨 Multifilter method for determining relative spectral sensitivity functions of photoelectric detectors, M J. Opt.

Soc. Am., vo1. 50, no· 10, pp· 992-998, I960· [13] International Commission on IlluminationSoc. Am., Vo1. 50, no · 10, pp · 992-998, I960 · [13] International Commission on Illumination

第28頁 491938 五、發明說明(24) (CIE),Determination of the Spectral Respons i v i ty of Optical Radiation Detectors, Pubication CIE No. 64, Paris, France, 1982.Page 28 491938 V. Description of the Invention (24) (CIE), Determination of the Spectral Respons i v i ty of Optical Radiation Detectors, Pubication CIE No. 64, Paris, France, 1982.

[14] G. W. Chang and Y. C. Chen, "Automatic spectral measurement system for col or video cameras,丨丨 IEEE Trans. Consumer Electronics, vo 1. 45, no· 1, 225-235, 1999.[14] G. W. Chang and Y. C. Chen, " Automatic spectral measurement system for col or video cameras, 丨 丨 Trans. Consumer Electronics, vo 1. 45, no · 1, 225-235, 1999.

[15] G. W. Chang and Y. C. Chen, "Spectral Respons i v i ty Estimator for Color Vision Systems : Filter Selection and Noise Effect,丨丨 Proceedings of National Sc i. Council,Part A, vo1. 13,no. 1 (to appear in Mar. 2001).[15] GW Chang and YC Chen, " Spectral Respons ivi ty Estimator for Color Vision Systems: Filter Selection and Noise Effect, 丨 丨 Proceedings of National Sc i. Council, Part A, vo1. 13, no. 1 (to appear in Mar. 2001).

[16] W. N. Sproson, Color Science in Television and Display Systems, Adam Hilger, Bristol, 1983.[16] W. N. Sproson, Color Science in Television and Display Systems, Adam Hilger, Bristol, 1983.

[17] G. E. Healey and R. Kondepudy, "Radiometric CCD earnera calibration and noise estimation," IEEE Trans. Pattern Anal. Mach. Intell·,vo1. 16,no. 3, pp· 267-276, 1994· [18] G. H. Golub and C. F. Van Loan, Matrix Computations, 2nd ed., Baltimore and London: John Hopkins Univ. Press, 1989.[17] GE Healey and R. Kondepudy, " Radiometric CCD earnera calibration and noise estimation, " IEEE Trans. Pattern Anal. Mach. Intell ·, vo1. 16, no. 3, pp · 267-276, 1994 · [ 18] GH Golub and CF Van Loan, Matrix Computations, 2nd ed., Baltimore and London: John Hopkins Univ. Press, 1989.

[19] C. L· Lawson and R. J. Hanson, Solving Least Squares Problems, NJ: Prentice-Hall, 1974.[19] C. L. Lawson and R. J. Hanson, Solving Least Squares Problems, NJ: Prentice-Hall, 1974.

[20] V. Oppenhe i m and R. W. Schafer, Discrete-Time[20] V. Oppenhe i m and R. W. Schafer, Discrete-Time

第29頁 491938 五、發明說明(25)Page 29 491938 V. Description of the invention (25)

Signal Processing, Prentice Hall, NJ, 1989.Signal Processing, Prentice Hall, NJ, 1989.

[21] G. Wyszecki and W. S. Stiles, Color Science -Concepts and Methods, Quantitative Data and Formulae, John Wiley and Sons, NY, 1982.[21] G. Wyszecki and W. S. Stiles, Color Science -Concepts and Methods, Quantitative Data and Formulae, John Wiley and Sons, NY, 1982.

[22] G. W. Chang, "Spectral Re spons i v i ty Estimation and Colorimetric Characterization for Machine Vision Systems, n (機械視覺系統之光、譜響應估 測與色彩模式特徵化)Ph.D. Dissertation, National Tsing Hua Univ·, June 200 0·(未公開,預計20 02 年6 月 公開)[22] GW Chang, " Spectral Re spons ivi ty Estimation and Colorimetric Characterization for Machine Vision Systems, n (Machine Vision System Light, Spectral Response Estimation, and Color Mode Characterization) Ph.D. Dissertation, National Tsing Hua Univ ·, June 200 0 · (Unpublished, expected to be released in June 2002)

第30頁 491938 圖式簡單說明 圖2 圖3 圖4 圖5 圖6 圖7 圖8 圖1 在多通道濾波(MCF)系統中的光譜響應特徵化過程。 系統光源表面光譜輻射功率分佈之一較佳實現例。 QRCP方法在子集合選擇(su]3Set selection)上的效 應。 QRCP-based濾波器選擇演算法流程圖。 以QRCP-based方法所選擇的濾波器組之光譜穿 分佈。 干 估測所得的Sony XC711攝影機光譜響應。 相對於測試色光(TCL)編號i至72的規一化均方 差(NRMSE)分佈。 根决 在Λ旒雜訊比為35 dB之下,來自(a)選擇法} 擇法2,(C)選擇法3,與(d)QRCp_based選擇法’ 二 之估測的光譜響應之比較。 斤件到 表1 表2 表3 表4 表5 不同濾波器選擇的結果(以減波哭 示)。 /應及。口京引編旒的集合表 QRcp〜based方法之性能評估表。 =自不同濾波器選擇所得的條件數。 檢驗雜訊效應的模擬結果。 來自不同濾波器選擇方法所P从上 >、,始 差。 无所侍的光譜響應估測誤Page 30 491938 Brief description of the drawings Figure 2 Figure 3 Figure 4 Figure 5 Figure 6 Figure 7 Figure 8 Figure 1 The spectral response characterization process in a multi-channel filtering (MCF) system. A preferred implementation example of the spectral radiation power distribution on the surface of the system light source. Effect of QRCP method on sub-set selection (su) 3Set selection. QRCP-based filter selection algorithm flowchart. The spectral penetration distribution of the filter bank selected by the QRCP-based method. Estimate the spectral response of the Sony XC711 camera. Normalized mean square error (NRMSE) distribution with respect to test color light (TCL) numbers i to 72. Based on the comparison of the estimated spectral response of the Λ 旒 noise ratio of 35 dB from (a) selection method} selection method 2, (C) selection method 3, and (d) QRCp_based selection method 'two. Parts to Table 1 Table 2 Table 3 Table 4 Table 5 The results of different filter selection (indicated by wave reduction). / Yes. A collection of tables compiled by Koukyo cited QRcp ~ based method performance evaluation table. = Number of conditions obtained from different filter selections. Verify the simulation results of noise effects. From the different filter selection methods, P is from the above > Miscalculated spectral response estimation

Claims (1)

491938 六 申睛專利範圍 一 ---------- κ 一種量測數位取像裝置光譜響應之多通道法 設計方法,其中多通道渡波系統μ 波系統的 之 過 -組特別選定且裝設在不同通道的光譜濾波2 =源與 光學系統’該光源所發出的轄射光於不同形成 該組在相異通道的濾波器產生不同指定的々:間y刀別通 :測的取像裝置;,玄多通道渡波系統的設 波器之選擇方法,該方法之組成步驟如下:去為该組濾 所有待選的滤波器分別標上索引編號,並 索引編號來建立一個以行向量形式表示的491938 Six patents for patent application 1 ---------- κ A multi-channel design method for measuring the spectral response of a digital imaging device, in which the over-group of the multi-channel crossing wave system μ-wave system is specially selected and Spectral filtering installed in different channels 2 = Source and optical system 'The emitted light emitted by this light source is different in the filters that form the group in different channels, and produces different specifications: 间: y, 刀, 测: measured images Device; A method of selecting a wave setter for a mysterious multi-channel ferry wave system. The composition steps of the method are as follows: to index all the filters to be selected for the group, and index them to create a row vector form. Expressed (2 ) 蒐集該面光源通過所有待 色刺激之光譜輻射分佈的集合 矩陣; 選擇的光譜濾波器所產生的 ,來形成一個巨大的色刺激 (3) 對該色刺激矩陣進行奇異值分解之運算, 對應於所有右奇異向量所形成的右奇異矩陣; (4) 檢驗該色刺激矩陣之矩陣的秩是否大於或等於在通 上濾,器的總數之條件是否成立;若為是,則進行下一 驟;若為非’則表示無法選擇適當的濾波器集合 此方法之進行;(2) Collect the aggregate matrix of the spectral radiation distribution of the surface light source through all the stimuli to be colored; Generated by the selected spectral filter to form a huge color stimulus (3) Perform the singular value decomposition operation on the color stimulus matrix , Corresponding to the right singular matrix formed by all right singular vectors; (4) check whether the rank of the matrix of the color stimulus matrix is greater than or equal to the filter on the pass, and the condition of the total number of filters is true; if yes, proceed to the following One step; if not, it means that the appropriate filter set cannot be selected for this method; (5)取該右奇異矩陣内前面與在通道上濾波器的總數相同 數目的行,來建構該右奇異矩陣之子矩陣,稱之為右 子矩陣; 〃 (6)取,右奇異子矩陣的轉置矩陣之直交三角形分解與行 轉換運算’並儲存該運算所產生排列矩陣;(5) Take the same number of rows in the right singular matrix as the previous total number of filters on the channel to construct the submatrix of the right singular matrix, called the right submatrix; 〃 (6) Take the The orthogonal triangle decomposition and row conversion operation of the transposed matrix 'and stores the permutation matrix generated by the operation; 第32頁 491938 六、申請專利範圍 (7 )將該濾波器索引向量之轉置所形成的列向量與該排列 矩陣相乘’其結果係為一個轉置的濾、波為索引向量做行排 列轉換所形成的列向量; (8 )取該由行排列轉換所形成的列向量之前面與在通道Λ 濾波器的總數相同數目的元素所形成之向量,稱之為所遽 擇的濾波器索引向量,該向量内所有的元素即為所選擇的 濾波器索引編號,因此我們完成了濾波器選擇的工作,邡 即完成了以多通道濾波器集合為基礎的光學系統之設計工 作0Page 32 491938 VI. Patent application scope (7) Multiply the column vector formed by the transposition of the filter index vector with the permutation matrix. The result is a transposed filter, and the waves are arranged in rows for the index vector. The column vector formed by the conversion; (8) Take the vector formed by the same number of elements in front of the column vector formed by the row permutation conversion as the total number of filters in the channel Λ, and call it the selected filter index Vector, all elements in the vector are the selected filter index number, so we have completed the filter selection work, and have completed the design of the optical system based on the multi-channel filter set. 2 ·根據申請專利範圍第1項所述之多通道濾波系統的設計 方法’其中所選擇的光譜濾波器之集合得分別安裝在同一 可,動的圓盤裝置,同時在空間分佈上形成不同的通道, 使知共同的系統光源所發出的輻射光在不同的時間穿透不 同的濾波器別產生對應的色刺激入射至待測的取像裝 根據申請專利範圍第1項所述 3. ^ . ., 不π述又夕通道濾波系統的12 · According to the design method of the multi-channel filtering system described in item 1 of the scope of the patent application, 'The selected set of spectral filters must be installed on the same movable disk device, respectively, and different spatial distributions are formed at the same time. Channel, so that the radiant light emitted by the common system light source penetrates different filters at different times to generate corresponding color stimuli and is incident on the image acquisition device to be measured according to item 1 of the patent application scope 3. ^. ., Not described 1 of the channel filter system 方法,其中所選擇的據波器數目應在1至10。之間 4.根據申請專利範圍第1項或第2頊所、十' —夕 統的設計方法,其中在夕項所述之多通道渡波 目應大於或等於所選擇的濾波器數 所選擇的濾波器集合之外,1 θ在通道上除了 : 卜其餘通道得安裝其他任一jMethod, in which the number of selected wave receivers should be between 1 and 10. 4. According to the design method of the scope of the application for patents No. 1 or No. 2 and No. 10, where the multi-channel crossing wave described in the item No. should be greater than or equal to the number of filters selected In addition to the filter set, 1 θ is on the channel in addition to: Any other channel j must be installed 第33頁 491938 六、申請專利範圍 的濾波器。 5.根據申請專利範圍第1項或第2項所述之多通道濾波系 統的設計方法,其中在多通道濾波系統裝置上,通道的數 目應在1 至2 0 0之間。 Φ Bill 第34頁Page 33 491938 VI. Patent application scope filter. 5. The design method of the multi-channel filtering system according to item 1 or 2 of the scope of the patent application, in which the number of channels on the multi-channel filtering system device should be between 1 and 200. Φ Bill p. 34
TW89125256A 2000-11-28 2000-11-28 Method of designing a multichannel filtering system for measuring digital camera's spectral responsivities TW491938B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
TW89125256A TW491938B (en) 2000-11-28 2000-11-28 Method of designing a multichannel filtering system for measuring digital camera's spectral responsivities

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
TW89125256A TW491938B (en) 2000-11-28 2000-11-28 Method of designing a multichannel filtering system for measuring digital camera's spectral responsivities

Publications (1)

Publication Number Publication Date
TW491938B true TW491938B (en) 2002-06-21

Family

ID=21662099

Family Applications (1)

Application Number Title Priority Date Filing Date
TW89125256A TW491938B (en) 2000-11-28 2000-11-28 Method of designing a multichannel filtering system for measuring digital camera's spectral responsivities

Country Status (1)

Country Link
TW (1) TW491938B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI418207B (en) * 2006-04-28 2013-12-01 Electro Scient Ind Inc Improving image quality via multi-wavelength light

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI418207B (en) * 2006-04-28 2013-12-01 Electro Scient Ind Inc Improving image quality via multi-wavelength light

Similar Documents

Publication Publication Date Title
US11193830B2 (en) Spectrocolorimeter imaging system
Vora et al. Digital color cameras—2—Spectral response
Farrell et al. Digital camera simulation
KR20150136585A (en) High accuracy imaging colorimeter by special designed pattern closed-loop calibration assisted by spectrograph
CN101933321A (en) Image sensor apparatus and method for scene illuminant estimation
JP2011528866A (en) Universally packed pixel array camera system and method
Helling et al. Algorithms for spectral color stimulus reconstruction with a seven-channel multispectral camera
TW201106706A (en) Spatially-varying spectral response calibration data
Farrell et al. Sensor calibration and simulation
Fiorentin et al. Calibration of digital compact cameras for sky quality measures
TW491938B (en) Method of designing a multichannel filtering system for measuring digital camera's spectral responsivities
Pointer et al. Practical camera characterization for colour measurement
Raza et al. Accuracy of hyperspectral imaging systems for color and lighting research
Shen et al. Colorimetric and spectral characterization of a color scanner using local statistics
Quan et al. Unified measure of goodness and optimal design of spectral sensitivity functions
WO2022242608A1 (en) Object preference memory color obtaining method and preference memory color standard color card
WO2011119268A2 (en) Optimal raw rgb determination for color calibration
Vora et al. Image capture: synthesis of sensor responses from multispectral images
Nyström Colorimetric and multispectral image acquisition using model-based and empirical device characterization
Keelan et al. Development of a perceptually calibrated objective metric of noise
Berns et al. Modifications of a sinarback 54 digital camera for spectral and high-accuracy colorimetric imaging: simulations and experiments
CN113758683A (en) Camera system post-irradiation spectral degradation evaluation method based on average color saturation
Fry et al. Noise Power Spectrum Scene-Dependency in Simulated Image Capture Systems
Getman et al. Crosstalk, color tint and shading correction for small pixel size image sensor
Klein Multispectral imaging: aberrations and acquisitions from different viewing positions

Legal Events

Date Code Title Description
GD4A Issue of patent certificate for granted invention patent
MM4A Annulment or lapse of patent due to non-payment of fees